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Table 3

Parameters for thermal reactions, desorptions, and photo-destruction.

Chemical reactions Reaction ratea ν0 (s-1) ν0(dif) (s-1) E (K) Ref.

H2CO+NH3 →NH2CH2OH k1 0.5 × 10-2 3.3 × 10-9 541 (Bossa et al. 2009b)
H2CO+CH3NH2 →CH3HNCH2OH k2 1.5 × 10-2 3.3 × 10-9 133 This work
CO2+2CH3NH2 →CH3NHCH3NHCOO k13 2 × 10-2 3.3 × 10-9 445 (Bossa et al. 2009a)

Species Desorption ratea ν0 (s-1) E(K) Ref.

NH3 k5 3 × 1012 3008 (Sandford et al. 1993)
H2CO k4 1 × 1013 3250 (Theule et al. 2012)
CH3NH2 k8 3 × 1012 3008 (c)
NH2CH2OH k9 3 × 1012 6980 (Bossa et al. 2009b)
CH3HNCH2OH k11 3 × 1012 6980 (Bossa et al. 2009b)

Species Photo-destruction rateb σ (photon-1 cm2) Ref.

CH3HNCH2OH k12 3 × 10-19 this work
NH3 k6 3.2 × 10-20 (Cottin et al. 2003)
CH3NH2 k7 3.2 × 10-20 (Cottin et al. 2003)
H2CO k3 1.0 × 10-19 (Woodall et al. 2007)
NH2CH2OH k10 4.5 × 10-19 (Duvernay et al. 2010)
CO2 k14 3.8 × 10-19 (Cottin et al. 2003)

Notes. 

(a)

The rate coefficients are given in the form k = ν0exp( − E / T), where T is the ice temperature, ν0 the pre-exponential factor, and E the activation energy (reaction or desorption). The diffusion factor (ν0(dif)) is obtained using the method developed by Hasegawa et al. (1992).

(b)

Photo-destruction rates are written as k = σf, where σ represents the photo-destruction cross-section and f the interstellar ultraviolet radiation field.

(c)

Since NH and CHNH have the same desorption behaviour in our vacuum conditions, we used the same desorption rate.

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